Lecture 4: Introduction to Graph Theory and Consensus · Lecture 4: Introduction to Graph Theory and Consensus Richard M. Murray Caltech Control and Dynamical Systems 16 March 2009

Lecture 4: Introduction to

Graph Theory and Consensus

Richard M. Murray

Caltech Control and Dynamical Systems

16 March 2009Goals

• Introduce some motivating cooperative control problems

• Describe basic concepts in graph theory (review)

• Introduce matrices associated with graphs and related properties (spectra)

Based on CDS 270 notes by Reza Olfati-Saber (Dartmouth) and PhD thesis of Alex Fax (Northrop Grumman).

References

• R. Diestel, Graph Theory. Springer-Verlag, 2000.

• C. Godsil and G. Royle, Algebraic Graph Theory. Springer, 2001.

• R. A. Horn and C. R. Johnson, Matrix Analysis. Cambridge Univ Press,1987.

• R. Olfati-Saber and M, “Consensus Problems in Networks of Agents”, IEEE

Transactions on Automatic Control, 2004.

Richard M. Murray, Caltech CDSEECI, Mar 09

Cooperative Control Applications

Transportation

• Air traffic control

• Intelligent transportation systems

(ala California PATH project)

Military

• Distributed aperture imaging

• Battlespace management

Scientific

• Distributed aperture imaging

• Adaptive sensor networks (eg,

Adaptive Ocean Sampling Network)

Commercial

• Building sensor networks (related)

Non-vehicle based applications

• Communication networks

(routing, ...)

• Power grid, supply chain mgmt

2

Richard M. Murray, Caltech CDSISAT, Feb 09

Cooperative Control Systems Framework

Agent dynamics

Vehicle “role”

• encodes internal state +

relationship to current task

• Transition

Communications graph

• Encodes the system information flow

• Neighbor set

Communications channel

• Communicated information can be lost,

delayed, reordered; rate constraints

• ! = binary random process (packet loss)

Task

• Encode as finite horizon optimal control

• Assume task is coupled, env’t estimated

Strategy

• Control action for individual agents

Decentralized strategy

• Similar structure for role update

3

N i(x,!)

! ! A

!! = r(x,!)

G

M

JGCD, 2007

xi = f i(xi, ui) xi ! Rn, ui ! Rm

yi = hi(xi) yi ! Rq

yij [k] = !yi(tk ! "j) tk+1 ! tk > Tr

J =! T

0L(x,!, E(t), u) dt + V (x(T ),!(T )),

ui(x,!) = ui(xi,!i, y!i,!!i, E)

y!i = {yj1 , . . . , yjmi}jk ! N i mi = |N i|

{gij(x,!) : ri

j(x,!)}

!i ! =

!rij(x,!) g(x,!) = true

unchanged otherwise.

ui = ki(x,!)

Richard M. Murray, Caltech CDSEECI, Mar 09 4

Information Flow in Vehicle Formations

Example: satellite formation

• Blue links represent sensed

information

• Green links represent

communicated information

Sensed information

• Local sensors can see some subset of nearby vehicles

•Assume small time delays, pos’n/vel info only

Communicated information

•Point to point communications (routing OK)

•Assume limited bandwidth, some time delay

•Advantage: can send more complex information

Topological features

• Information flow (sensed or communicated) represents a directed graph

•Cycles in graph ! information feedback loops

Question: How does topological structure of information flow affectstability of the overall formation?

A Primer on Graph Theory

Richard M. Murray

Control and Dynamical SystemsCalifornia Institute of Technology

December 2007

Goals:

• Describe basic concepts in graph theory (review)

• Introduce matrices associated with graphs and related properties (spec-tra)

• Example: asymptotic concensus

Based on CDS 270 notes by Reza Olfati-Saber (Dartmouth) and PhD thesis of

Alex Fax (Northrop Grumman).

References:

1. R. Diestel, Graph Theory. Springer-Verlag, 2000.

2. C. Godsil and G. Royle, Algebraic Graph Theory. Springer, 2001.

3. R. A. Horn and C. R. Johnson, Matrix Analysis. Cambridge UnivPress, 1987.

1. Basic Definitions

Definition. A graph is a pair G = (V, E) that consists of a set of vertices Vand a set of edges E ! V " V:

• Vertices: vi # V

• Edges: eij = (vi, vj) # E

1

Example:

V = {1, 2, 3, 4, 5, 6}

E = {(1, 6), (2, 1), (2, 3), (2, 6), (6, 2), (3, 4),

(3, 6), (4, 3), (4, 5), (5, 1), (6, 1), (6, 2), (6, 4)}

Notation:

• Order of a graph = number of nodes: |V|

• vi and vj are adjacent if there exists e = (vi, vj)

• An adjacent node vj for a node vi is called a neighbor of vi

• Ni = set of all neighbors of vi

• G is complete if all nodes are adjacent

Undirected graphs

• A graph is undirected if eij ! E =" eji ! E

• Degree of a node: deg(vi) := |Ni|

• A graph is regular (or k-regular) if all vertices of a graph have the samedegree k

Directed graphs (digraph)

• Out-degree of vi: degout = number of edges eij = (vi, vj)

• In-degree of vi: degin = number of edges eki = (vk, vi)

Balanced graphs

• A graph is balanced if out-degree = in-degree at each node

2. Connectedness of Graphs

Paths

• A path is a subgraph ! = (V, E!) # G with distinct nodes V ={v1, v2, . . . , vm} and

E! := {(v1, v2), (v2, v3), . . . , (vm!1, vm)}.

• The length of ! is defined as |E!| = m $ 1.

2

• A cycle (or m-cycle) C = (V, EC) is a path (of length m) with an extraedge (vm, v1) ! E .

• The distance between two nodes v and w is the length of the shortestpath between them.

Connectivity of undirected graphs

• An undirected graph G is called connected if there exists a path !between any two distinct nodes of G.

• For a connected graph G, the length of the maximum distance betweentwo vertices is called the diameter of G.

• A graph with no cycles is called acyclic

• A tree is a connected acyclic graph

Connectivity of directed graphs

• A digraph is called strongly connected if there exists a directed path !between any two distinct nodes of G.

• A digraph is called weakly connected if there exists an undirected pathbetween any two distinct nodes of G.

3. Matrices Associated with a Graph

• The adjacency matrix A = [aij ] ! Rn!n of a graph G of order n isgiven by:

aij :=

!

1 if (vi, vj) ! E

0 otherwise

• The degree matrix of a graph as a diagonal n " n (n = |V|) matrix! = diag{degout(vi)} with diagonal elements equal to the out-degreeof each node and zero everywhere else.

• The Laplacian matrix L of a graph is defined as

L = ! # A

.• The row sums of the Laplacian are all 0.

A =

2

6

6

6

6

6

6

4

0 0 0 0 0 1

1 0 1 0 0 1

0 0 0 1 0 1

0 0 1 0 1 0

1 0 0 0 0 0

1 1 0 1 0 0

3

7

7

7

7

7

7

5

L =

2

6

6

6

6

6

6

4

1 0 0 0 0 !1

!1 3 !1 0 0 !1

0 0 2 !1 0 !1

0 0 !1 2 !1 0

!1 0 0 0 1 0

!1 !1 0 !1 0 3

3

7

7

7

7

7

7

5

3

4. Periodic Graphics and Weighted Graphs

Periodic and acyclic graphs

• A graph with the property that the set of all cycle lengths has a com-mon divisor k > 1 is called k-periodic.

• A graph without cycles is said to be acyclic.

Weighted graphs

• A weighted graph is graph (V, E) together with a map ! : E ! R

that assigns a real number wij = !(eij) called a weight to an edgeeij = (vi, vj) " E .

• The set of all weights associated with E is denoted by W.

• A weighted graph can be represented as a triplet G = (V, E ,W).

Weighted Laplacian

• In some applications it is natural to “normalize” the Laplacian by theoutdegree

• L := !!1L = I # A, where A = !!1A (weighted adjacency matrix).

5. Consensus protocols

Consider a collection of N agents that communicate along a set of undirectedlinks described by a graph G. Each agent has a state xi with initial valuexi(0) and together they wish to determine the average of the initial statesAve(x(0)) = 1/N

!

xi(0).

The agents implement the following consensus protocol:

xi ="

j"Ni

(xj # xi) = #|Ni|(xi # Ave(xNi))

which is equivalent to the dynamical system

x = u u = #Lx.

Proposition 1. If the graph is connected, the state of the agents convergesto x#

i = Ave(x(0)) exponentially fast.

• Proposition 1 implies that the spectra of L controls the stability (andconvergence) of the consensus protocol.

• To (partially) prove this theorem, we need to show that the eigenvaluesof L are all positive.

4

6. Gershgorin Disk Theorem

Theorem 2 (Gershgorin Disk Theorem). Let A = [aij ] ! Rn!n and definethe deleted absolute row sums of A as

ri :=n

!

j=1,j "=i

|aij | (1)

Then all the eigenvalues of A are located in the union of n disks

G(A) :=n"

i=1

Gi(A), with Gi(A) := {z ! C : |z " aii| # ri} (2)

Furthermore, if a union of k of these n disks forms a connected region thatis disjoint from all the remaining n " k disks, then there are precisely keigenvalues of A in this region.

Sketch of proof Let ! be an eigenvalue of A and let v be a correspond-ing eigenvector. Choose i such that |vi| = maxj |vj > 0. Since v is aneigenvector,

!vi =!

i

Aijvj =$ (! " aii)vi =!

i"=j

Aijvj

Now divide by vi %= 0 and take the absolute value to obtain

|! " aii| = |!

j "=i

aijvj | #!

j "=i

|aij | = ri

7. Properties of the Laplacian (1)

Proposition 3. Let L be the Laplacian matrix of a digraph G with maximumnode out–degree of dmax > 0. Then all the eigenvalues of A = "L are locatedin a disk

B(G) := {s ! C : |s + dmax| # dmax} (3)

that is located in the closed LHP of s-plane and is tangent to the imaginaryaxis at s = 0.

Proposition 4. Let L be the weighted Laplacian matrix of a digraph G.Then all the eigenvalues of A = "L are located inside a disk of radius 1 thatis located in the closed LHP of s-plane and is tangent to the imaginary axisat s = 0.

5

Theorem 5 (Olfati-Saber). Let G = (V, E , W ) be a weighted digraph oforder n with Laplacian L. If G is strongly connected, then rank(L) = n! 1.

Remarks:

• Proof for the directed case is standard

• Proof for undirected case is available in Olfati-Saber & M, 2004 (IEEETAC)

• For directed graphs, need G to be strongly connected and converse isnot true.

8. Proof of Consensus Protocol

x = !Lx L = ! ! A

Note first that the subspaced spanned by 1 = (1, 1, . . . , 1)T is an invari-ant subspace since L · 1 = 0 Assume that there are no other eigenvectorswith eigenvalue 0. Hence it su"ces to look at the convergence on the com-plementary subspace 1!.

Let ! be the disagreement vector

! = x ! Ave(x(0))1

and take the square of the norm of ! as a Lyapunov function candidate, i.e.define

V (!) = "!"2 = !T ! (4)

Di#erentiating V (!) along the solution of ! = !L!, we obtain

V (!) = !2!T L! < 0, #! $= 0, (5)

where we have used the fact that G is connected and hence has only 1zero eigenvalue (along 1). Thus, ! = 0 is globally asymptotically stableand ! % 0 as t % +&, i.e. x" = limt#+$ x(t) = "01 because "(t) ="0 = Ave(x(0)),#t > 0. In other words, the average–consensus is globallyasymptotically achieved.

9. Perron-Frobenius Theory

Spectral radius:

• spec(L) = {#1, . . . , #n} is called the spectrum of L.

• $(L) = |#n| = maxk |#k| is called the spectral radius of L

6

Theorem 6 (Perron’s Theorem, 1907). If A ! Rn!n is a positive matrix(A > 0), then

1. !(A) > 0;

2. r = !(A) is an eigenvalue of A;

3. There exists a positive vector x > 0 such that Ax = !(A)x;

4. |"| < !(A) for every eigenvalue " "= !(A) of A, i.e. !(A) is the uniqueeigenvalue of maximum modulus; and

5. [!(A)"1A]m # R as m # +$ where R = xyT , Ax = !(A)x, AT y =!(A)y, x > 0, y > 0, and xT y = 1.

Theorem 7 (Perron’s Theorem for Non–Negative Matrices). If A ! Rn!n

is a non-negative matrix (A % 0), then !(A) is an eigenvalue of A and thereis a non–negative vector x % 0, x "= 0, such that Ax = !(A)x.

10. Irreducible Graphs and Matrices

Irreducibility

• A directed graph is irreducible if, given any two vertices, there existsa path from the first vertex to the second. (Irreducible = stronglyconnected)

• A matrix is irreducible if it is not similar to a block upper triangularmatrix via a permutation.

• A digraph is irreducible if and only if its adjacency matrix is irre-ducible.

Theorem 8 (Frobenius). Let A ! Rn!n and suppose that A is irreducibleand non-negative. Then

1. !(A) > 0;

2. r = !(A) is an eigenvalue of A;

3. There is a positive vector x > 0 such that Ax = !(A)x;

4. r = !(A) is an algebraically simple eigenvalue of A; and

5. If A has h eigenvalues of modulus r, then these eigenvalues are alldistinct roots of "h & rh = 0.

7

11. Spectra of the Laplacian

Properties of L

• If G is strongly connected, the zero eigenvalue of L is simple.

• If G is aperiodic, all nonzero eigenvalues lie in the interior of the Ger-shgorin disk.

• If G is k-periodic, L has k evenly spaced eigenvalues on the boundaryof the Gershgorin disk.

12. Algebraic Connectivity

Theorem 9 (Variant of Courant-Fischer). Let A ! Rn!n be a Hermitianmatrix with eigenvalues !1 " !2 " · · · " !n and let w1 be the eigenvector ofA associated with the eigenvalue !1. Then

!2 = minx #= 0, x ! Cn,

x$w1

x"Ax

x"x= min

x"x = 1,x$w1

x"Ax (6)

Remarks:

• !2 is called the algebraic connectivity of L

• For an undirected graph with Laplacian L, the rate of convergence forthe consensus protocol is bounded by the second smallest eigenvalue!2

13. Cyclically Separable Graphs

Definition (Cyclic separability). A digraph G = (V, E) is cyclically sepa-rable if and only if there exists a partition of the set of edges E = %nc

k=1Ek

such that each partition Ek corresponds to either the edges of a cycle of thegraph, or a pair of directed edges ij and ji that constitute an undirectededge. A graph that is not cyclically separable is called cyclically inseparable.

Lemma 10. Let L be the Laplacian matrix of a cyclically separable digraphG and set u = &Lx, x ! Rn. Then

!ni=1 ui = 0,'x ! Rn and 1 = (1, . . . , 1)T

is the left eigenvector of L.

8

Proof. The proof follows from the fact that by definition of cyclic separabil-ity. We have

!n

!

i=1

ui =!

ij!E

(xj ! xi) =nc!

k=1

!

ij!Ek

(xj ! xi) = 0

because the inner sum is zero over the edges of cycles and undirected edgesof the graph.

• Provides a “conservation” principle for average consensus

14. Consensus on Balanced Graphs

Let G = (V, E) be a digraph. We say G is balanced if and only if the in–degreeand out–degree of all nodes of G are equal, i.e.

degout(vi) = degin(vi), "vi # V (7)

Theorem 11. A digraph is cyclically separable if and only if it is balanced.

Corollary 11.1. Consider a network of integrators with a directed informa-tion flow G and nodes that apply the consensus protocol. Then, ! = Ave(x)is an invariant quantity if and only if G is balanced.

Remarks

• Balanced graphs generalized undirected graphs and retain many keyproperties

9


Consensus Protocols for Balanced Graphs

5

31 2 4 5

678910

31 2 4 5

678910

(a) (b)31 2 4 5

678910

31 2 4 5

678910

(c) (d)

Figure 4: Four examples of balanced and strongly connected digraphs: (a) Ga, (b) Gb, (c)Gc, and (d) Gd satisfying.

as the number of the edges of the graph increases, algebraic connectivity (or !2) increases,and the settling time of the state trajectories decreases.

The case of a directed cycle of length 10, or Ga, has the highest over-shoot. In all fourcases, a consensus is asymptotically reached and the performance is improved as a functionof !2(Gk) for k ! {a, b, c, d}.

In Figure 6(a), a finite automaton is shown with the set of states {Ga, Gb, Gc, Gd} rep-resenting the discrete-states of a network with switching topology as a hybrid system. Thehybrid system starts at the discrete-state Gb and switches every T = 1 second to the nextstate according to the state machine in Figure 6(a). The continuous-time state trajectoriesand the group disagreement (i.e. """2) of the network are shown in Figure 6(b). Clearly, thegroup disagreement is monotonically decreasing. One can observe that an average-consensusis reached asymptotically. Moreover, the group disagreement vanishes exponentially fast.

Next, we present simulation results for the average-consensus problem with communica-tion time-delay for a network with a topology shown in Figure 7. Figure 8 shows the statetrajectories of this network with communication time-delay # for # = 0, 0.5#max, 0.7#max, #max

with #max = $/2!max(Ge) = 0.266. Here, the initial state is a random set of numbers withzero-mean. Clearly, the agreement is achieved for the cases with # < #max in Figures 8(a),(b), and (c). For the case with # = #max, synchronous oscillations are demonstrated in Figure8(d). A third-order Pade approximation is used to model the time-delay as a finite-orderLTI system.

12 Conclusions

We provided the convergence analysis of a consensus protocol for a network of integratorswith directed information flow and fixed/switching topology. Our analysis relies on severaltools from algebraic graph theory, matrix theory, and control theory. We established a con-

22

0 5 10 15!20

!10

0

10Algebraic Connectivity=0.191

time( sec)

node v

alu

e

0 5 10 150

100

200

300

time( sec)

dis

agre

em

ent

0 5 10 15!20

!10

0


time( sec)

node v

alu

e

0 5 10 150

100

200

300

time( sec)dis

agre

em

ent

(a) (b)

0 5 10 15!20

!10

0


time( sec)

node v

alu

e

0 5 10 150

100

200

300

time( sec)

dis

agre

em

ent

0 5 10 15!20

!10

0


time( sec)

node v

alu

e

0 5 10 150

100

200

300

time( sec)

dis

agre

em

ent

(c) (d)

Figure 5: For examples of balanced and strongly connected digraphs: (a) Ga, (b) Gb, (c) Gc,and (d) Gd satisfying.

nection between the performance of a linear consensus protocol and the Fiedler eigenvalue ofthe mirror graph of a balanced digraph. This provides an extension of the notion of algebraicconnectivity of graphs to algebraic connectivity of balanced digraphs. A simple disagreementfunction was introduced as a Lyapunov function for the group disagreement dynamics. Thiswas later used to provide a common Lyapunov function that allowed convergence analysis ofan agreement protocol for a network with switching topology. A commutative diagram wasgiven that shows the operations of taking Laplacian and symmetric part of a matrix commutefor adjacency matrix of balanced graphs. Balanced graphs turned out to be instrumental insolving average-consensus problems.

For undirected networks with fixed topology, we gave su!cient and necessary condi-tions for reaching an average-consensus in presence of communication time-delays. It was

23


Other Uses of Consensus Protocols

Computation of other functions besides the average

• Can adopt the basic approach to compute max, min, etc

• Chandy/Charpentier: can compute superidempotent functions:

Basic idea: local conservation implies global conservation

• Can extend these cases to handle splitting and rejoining as well

Distributed Kalman filtering

• Maintain local estimates of global average and covariance

• Need to be careful about choosing rates of convergence

6

f(X ! Y ) = f(f(X) ! Y )

8 Reza Olfati-Saber

with a state (ei, qi) ! R2m, input ui, and output qi. This filter is used forinverse-covariance consensus that calculates Si column-wise for node i byapplying the filter on columns of H !

iR"1i Hi as the inputs of node i. The

matrix version of this filter can take H !iR

"1i Hi as the input.

Fig. 2 shows the architecture of each node of the sensor network for dis-tributed Kalman filtering. Note that consensus filtering is performed with thesame frequency as Kalman filtering. This is a unique feature that completelydistinguishes our algorithm with some related work in [30, 33].

Sensor

Data

Covariance

Data

Low-Pass

Consensus Filter

Band-Pass

Consensus Filter

Micro

Kalman

Filter

(µKF)

Node i

x

(a) (b)

Fig. 2. Node and network architecture for distributed Kalman filtering: (a) archi-tecture of consensus filters and µKF of a node and (b) communication patternsbetween low-pass/band-pass consensus filters of neighboring nodes.

5 Simulation Results

In this section, we use our consensus filters jointly with the update equationof the micro-Kalman filter of each node to obtain an estimate of the positionof a moving object in R2 that (approximately) goes in circles. The outputmatrix is Hi = I2 and the state of the process dynamics is 2-dimensionalcorresponding to the continuous-time system

x = A0x + B0w

8 Reza Olfati-Saber

with a state (ei, qi) ! R2m, input ui, and output qi. This filter is used forinverse-covariance consensus that calculates Si column-wise for node i byapplying the filter on columns of H !

iR"1i Hi as the inputs of node i. The

matrix version of this filter can take H !iR

"1i Hi as the input.

Fig. 2 shows the architecture of each node of the sensor network for dis-tributed Kalman filtering. Note that consensus filtering is performed with thesame frequency as Kalman filtering. This is a unique feature that completelydistinguishes our algorithm with some related work in [30, 33].

Sensor

Data

Covariance

Data

Low-Pass

Consensus Filter

Band-Pass

Consensus Filter

Micro

Kalman

Filter

(µKF)

Node i

x

(a) (b)

Fig. 2. Node and network architecture for distributed Kalman filtering: (a) archi-tecture of consensus filters and µKF of a node and (b) communication patternsbetween low-pass/band-pass consensus filters of neighboring nodes.

5 Simulation Results

In this section, we use our consensus filters jointly with the update equationof the micro-Kalman filter of each node to obtain an estimate of the positionof a moving object in R2 that (approximately) goes in circles. The outputmatrix is Hi = I2 and the state of the process dynamics is 2-dimensionalcorresponding to the continuous-time system

x = A0x + B0w

Richard M. Murray, Caltech CDSEECI, Mar 09 7

Robustness

What happens if a single node “locks up”

Different types of robustness (Gupta, Langbort & M)

• Type I - node stops communicating (stopping failure)

• Type II - node communicates constant value

• Type III - node computes incorrect function (Byzantine failure)

Related ideas: delay margin for multi-hop models (Jin and M)

• Improve consensus rate through multi-hop, but create sensitivity to communcations delay

• Single node can change entirevalue of the consenus

• Desired effect for “robust”behavior: "xI = #/N

x1(0) = 4

x2(0) = 9

x3(0) = 6 x4(t) = 0

X5(t) = 6

x6(t) = 5

Gupta, Langbort and M

CDC 06


Summary

Graphs

• Directed, undirected, connected, strongly complete

• Cyclic versus acyclic; irreducible, balanced

Graph Laplacian

• L = ! - A

• Spectral properties related to connectivity of graph

• # zero eigenvalues = # strongly connected components

• Second largest nonzero eigenvalue ~ weak links

Spectral Properties of Graphs

• Gershgorin’s disk theorem

• Perron-Frobenius theory

Examples

• Consensus problems, distributed computing

• Distributed control (coming up next...)

8

Documents

Lecture 4: Introduction to Graph Theory and Consensus · Lecture 4: Introduction to Graph Theory and Consensus Richard M. Murray Caltech Control and Dynamical Systems 16 March 2009